Chemistry:Lead zirconate titanate
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| Names | |
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| IUPAC name
Lead zirconium titanate
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| Other names
Lead zirconium titanate
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| Identifiers | |
3D model (JSmol)
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| EC Number |
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PubChem CID
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| Properties | |
| Pb[Zr xTi 1-x]O 3 (0 ≤ x ≤ 1) | |
| Molar mass | 303.065 to 346.4222 g/mol |
| Hazards | |
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| GHS Signal word | Danger |
| H302, H332, H360, H373, H410 | |
| P201, P202, P260, P261, P264, P270, P271, P273, P281, P301+312, P304+312, P304+340, P308+313, P312, P314, P330, P391, P405, P501 | |
Except where otherwise noted, data are given for materials in their standard state (at 25 °C [77 °F], 100 kPa). | |
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| Infobox references | |
Lead zirconate titanate, also called lead zirconium titanate and commonly abbreviated as PZT, is an inorganic compound with the chemical formula Pb[Zr
xTi
1-x]O
3 (0 ≤ x ≤ 1). It is a ceramic perovskite material that shows a marked piezoelectric effect, meaning that the compound changes shape when an electric field is applied. It is used in a number of practical applications such as ultrasonic transducers and piezoelectric resonators. It is a white to off-white solid.
Lead zirconium titanate was first developed around 1952 at the Tokyo Institute of Technology. Compared to barium titanate, a previously discovered metallic-oxide-based piezoelectric material, lead zirconium titanate exhibits greater sensitivity and has a higher operating temperature. Piezoelectric ceramics are chosen for applications because of their physical strength, chemical inertness and their relatively low manufacturing cost. PZT ceramic is the most commonly used piezoelectric ceramic because it has an even greater sensitivity and higher operating temperature than other piezoceramics.[1] Recently, there has been a large push towards finding alternatives to PZT due to legislations in many countries restricting the use of lead alloys and compounds in commercial products.[2]
Electroceramic properties
Being piezoelectric, lead zirconate titanate develops a voltage (or potential difference) across two of its faces when compressed (useful for sensor applications), and physically changes shape when an external electric field is applied (useful for actuator applications). The relative permittivity of lead zirconate titanate can range from 300 to 20000, depending upon orientation and doping.[citation needed]
Being pyroelectric, this material develops a voltage difference across two of its faces under changing temperature conditions; consequently, lead zirconate titanate can be used as a heat sensor. Lead zirconate titanate is also ferroelectric, which means that it has a spontaneous electric polarization (electric dipole) that can be reversed in the presence of an electric field.
The material features an extremely large relative permittivity at the morphotropic phase boundary (MPB) near x = 0.52.[3]
Some formulations are ohmic until at least 250 kV/cm (25 MV/m), after which current grows exponentially with field strength before reaching avalanche breakdown; but lead zirconate titanate exhibits time-dependent dielectric breakdown — breakdown may occur under constant-voltage stress after minutes or hours, depending on voltage and temperature, so its dielectric strength depends on the time scale over which it is measured.[4] Other formulations have dielectric strengths measured in the 8–16 MV/m range.[5]
Uses
Lead zirconate titanate-based materials are components of ceramic capacitors and STM/AFM actuators (tubes).
Lead zirconate titanate is used to make ultrasound transducers and other sensors and actuators, as well as high-value ceramic capacitors and FRAM chips. Lead zirconate titanate is also used in the manufacture of ceramic resonators for reference timing in electronic circuitry. Anti-flash goggles featuring PLZT protect aircrew from burns and blindness in case of a nuclear explosion.[6] The PLZT lenses could turn opaque in less than 150 microseconds.
Commercially, it is usually not used in its pure form, rather it is doped with either acceptors, which create oxygen (anion) vacancies, or donors, which create metal (cation) vacancies and facilitate domain wall motion in the material. In general, acceptor doping creates hard lead zirconate titanate, while donor doping creates soft lead zirconate titanate. Hard and soft lead zirconate titanate generally differ in their piezoelectric constants. Piezoelectric constants are proportional to the polarization or to the electrical field generated per unit of mechanical stress, or alternatively is the mechanical strain produced by per unit of electric field applied. In general, soft lead zirconate titanate has a higher piezoelectric constant, but larger losses in the material due to internal friction. In hard lead zirconate titanate, domain wall motion is pinned by the impurities, thereby lowering the losses in the material, but at the expense of a reduced piezoelectric constant.
Varieties
One of the commonly studied chemical composition is PbZr
0.52Ti
0.48O
3. The increased piezoelectric response and poling efficiency near to x = 0.52 is due to the increased number of allowable domain states at the MPB. At this boundary, the 6 possible domain states from the tetragonal phase ⟨100⟩ and the 8 possible domain states from the rhombohedral phase ⟨111⟩ are equally favorable energetically, thereby allowing a maximum 14 possible domain states.
Like structurally similar lead scandium tantalate and barium strontium titanate, lead zirconate titanate can be used for manufacture of uncooled staring array infrared imaging sensors for thermographic cameras. Both thin film (usually obtained by chemical vapor deposition) and bulk structures are used. The formula of the material used usually approaches Pb
1.1(Zr
0.3Ti
0.7)O
3 (called lead zirconate titanate 30/70). Its properties may be modified by doping it with lanthanum, resulting in lanthanum-doped lead zirconium titanate (lead zirconate titanate, also called lead lanthanum zirconium titanate), with formula Pb
0.83La
0.17(Zr
0.3Ti
0.7)
0.9575O
3 (lead zirconate titanate 17/30/70).[7]
See also
References
- ↑ "What is "Lead zirconium titanate"?". APC International. https://www.americanpiezo.com/piezo-theory/pzt.html.
- ↑ Bell, Andrew J.; Deubzer, Otmar (August 2018). "Lead-free piezoelectrics—The environmental and regulatory issues" (in en). MRS Bulletin 43 (8): 581–587. doi:10.1557/mrs.2018.154. ISSN 0883-7694. http://eprints.whiterose.ac.uk/135355/1/Aug18_Bell%20and%20Deubzer%20AM.pdf.
- ↑ Rouquette, J.; Haines, J.; Bornand, V.; Pintard, M.; Papet, Ph; Bousquet, C.; Konczewicz, L.; Gorelli, F. A. et al. (2004). "Pressure tuning of the morphotropic phase boundary in piezoelectric lead zirconate titanate". Physical Review B 70 (1): 014108. doi:10.1103/PhysRevB.70.014108.
- ↑ Moazzami, Reza; Hu, Chenming; Shepherd, William H. (September 1992). "Electrical Characteristics of Ferroelectric Lead zirconate titanate Thin Films for DRAM Applications". IEEE Transactions on Electron Devices 39 (9): 2044. doi:10.1109/16.155876. http://www.eecs.berkeley.edu/~hu/PUBLICATIONS/Hu_papers/Hu_JNL/HuC_JNL_114.pdf.
- ↑ Andersen, B.; Ringgaard, E.; Bove, T.; Albareda, A.; Pérez, R. (2000). "Performance of Piezoelectric Ceramic Multilayer Components Based on Hard and Soft Lead zirconate titanate". Proceedings of Actuator 2000: 419–422. https://www.researchgate.net/publication/237514139.
- ↑ Cutchen, J. Thomas; Harris, James O. Jr.; Laguna, George R. (1975). "PLZT electrooptic shutters: applications". Applied Optics 14 (8): 1866–1873. doi:10.1364/AO.14.001866. PMID 20154933. http://www.opticsinfobase.org/ao/abstract.cfm?URI=ao-14-8-1866.
- ↑ Liu, W.; Jiang, B.; Zhu, W. (2000). "Self-biased dielectric bolometer from epitaxially grown Pb(Zr,Ti)O3 and lanthanum-doped Pb(Zr,Ti)O3 multilayered thin films". Applied Physics Letters 77 (7): 1047–1049. doi:10.1063/1.1289064.
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